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Section  2.2  Differential  Equations  of  Physical  Systems          53
                       Nomenclature

                          3  Through-variable:  F  =  force, T  = torque, i  =  current, Q =  fluid volumetric flow
                            rate, q  =  heat  flow rate.
                          CI Across-variable:  v  = translational  velocity, a>  =  angular velocity, v  =  voltage,
                            P  =  pressure, 9" =  temperature.
                         •  Inductive  storage:  L  =  inductance, \/k  -  reciprocal translational  or rotational
                            stiffness, I  = fluid  inertance.
                         •  Capacitive  storage: C  =  capacitance, M  -  mass, J  =  moment  of inertia, C/  =  fluid
                            capacitance, C,  = thermal  capacitance.
                         3  Energy  dissipators:  R  =  resistance, b =  viscous friction, R f  = fluid resistance,
                            R,  = thermal resistance.
                          The symbol  v is used  for both  voltage  in electrical circuits and  velocity in trans-
                       lational mechanical systems and is distinguished within the context  of each  differen-
                       tial equation. For mechanical systems, one uses Newton's laws; for electrical systems,
                       Kirchhoff s voltage  laws. For  example, the  simple  spring-mass-damper  mechanical
                       system shown in Figure 2.2(a)  is described  by Newton's second law of motion.  (This
                       system could represent, for  example, an automobile  shock  absorber.) The  free-body
                       diagram  of the mass M is shown in Figure 2.2(b). In  this spring-mass-damper  exam-
                       ple,  we  model  the  wall  friction  as  a  viscous  damper,  that  is, the  friction  force  is
                       linearly proportional to the velocity  of the mass. In reality  the friction  force may be-
                       have  in a more complicated  fashion. For example, the wall friction  may behave  as a
                       Coulomb  damper. Coulomb  friction,  also known  as dry friction, is a nonlinear  func-
                       tion  of  the  mass velocity  and  possesses  a  discontinuity  around  zero  velocity. For  a
                       well-lubricated, sliding  surface,  the  viscous  friction  is appropriate  and  will be  used
                       here  and  in  subsequent  spring-mass-damper  examples. Summing  the  forces  acting
                       on  M and  utilizing Newton's  second  law yields


                                            M-~-    +  b ^ -  + ky(t)  =  r(t%             (2.1)
                                               dt*       dt

                       where k is the spring constant  of the ideal spring and b is the friction  constant. Equa-
                       tion  (2.1) is a second-order linear constant-coefficient  differential  equation.






                       Wall
                                    5    _  i
                       friction,  b
                               \   Mass
                                    M
                                    1
      FIGURE  2.2
      (a) Spring-mass-              / • ( / )
      damper system.               Force
      (b) Free-body
      diagram.                      in)
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